Step 1: Use the common log form of the belt friction equation.
Textbooks often write $\dfrac{\mu\theta}{2.3026} = \log_{10}\left(\dfrac{T_1}{T_2}\right)$, which avoids working with $e^x$ directly.
The governing angle is the smaller wrap of $170^{\circ}$, since that pulley reaches the friction limit first.
$\theta = 170 \times \dfrac{3.14}{180} = 2.971$ rad, so $\mu\theta = 0.30 \times 2.971 = 0.8913$.
Step 2: Solve for the tension ratio.
$\log_{10}\left(\dfrac{T_1}{T_2}\right) = \dfrac{0.8913}{2.3026} = 0.3870$.
$\dfrac{T_1}{T_2} = 10^{0.3870} = 2.438$, so $T_1 = 2.438 \times 250 = 609.6$ N.
Step 3: Bring in the belt speed and net pulling force.
Belt speed $v = \dfrac{\pi D N}{60} = \dfrac{3.14 \times 0.6 \times 500}{60} = 15.70$ m/s.
Net driving force $= T_1 - T_2 = 609.6 - 250 = 359.6$ N.
Step 4: Compute the power.
$P = 359.6 \times 15.70 = 5646$ W, which is 5.65 kW.
Final Answer:
Rounded to the nearest listed value, the power transmitted is 5.6 kW, matching option B.
\[ \boxed{P \approx 5.6\ \text{kW}} \]